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Question: Is the potential energy of an electron in a hydrogen atom well defined? Is the kinetic energy well defined? Justify your answers. (You need not actually calculate uncertainties.)

Short Answer

Expert verified

Answer

Neither the potential energy nor the kinetic energy for an electron in a hydrogen atom is well defined.

Step by step solution

01

 Concept

The Heisenberg Uncertainty Principle states that the momentum and the position of a particle cannot be measured simultaneously with arbitrary accuracy. For an uncertainty in position (x)and the uncertainty in momentum (p), the uncertainty principle is given as-
x=ph2

02

 Solution

We know that the potential energy of an electron in a hydrogen atom is a function of its position r

U(r)=-e2(4πε0)r......(1)

However, the position of the electron cannot be defined accurately. According to the Heisenberg uncertainty principle, there is an uncertainty in position,r .This uncertainty in position leads to an uncertainty in the potential energy.
U=e24πε0r2r

Similarly, the kinetic energy is a function of both rotational and the radial momentum operator P^rad=-ihrddrr

knowing that the angular momentum takes the values
L=l(l+1)hforl=0,1,2.....,n-1, we have
KE^=p2rad^2m+L22mr2
=12m-ihrddrr2+l(l+1)h22mr2=-h22m1r2ddrr2ddr+l(l+1)h22mr2K.EradK.Erot

Which agrees with equation (30).

So, we can see the precise definition of the kinetic energy requires the precise value of both the radial momentum and position at the same time, which is not possible, by the virtue of the uncertainty principle.

Therefore, we conclude that neither the potential energy nor the kinetic energy can be well defined for an electron in a hydrogen atom

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Most popular questions from this chapter

A particle is subject to a potential energy that has an essentially infinitely high wall at the origin, like the infinite well, but for positive values of x is of the form U(x)= -b/ x, where b is a constant

(a) Sketch this potential energy.

(b) How much energy could a classical particle have and still be bound by such a potential energy?

(c) Add to your sketch a plot of E for a bound particle and indicate the outer classical tuning point (the inner being the origin).

(d) Assuming that a quantum-mechanical description is in order, sketch a plausible ground-state wave function, making sure that your function's second derivative is of the proper sign when U(x)is less than E and when it is greater.

Determine the Fourier transform A(k)of the oscillatory functionf(x) ) and interpret the result. (The identity cos(k0x)=12(e+ik0+eik0)may be useful.)

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